In the \(e^{+}e^{-}\rightarrow p\bar{p}\)  process, the BaBar collaboration observed a rapid rise of the cross section near threshold, followed by a plateau around 200 MeV above threshold [1]}. The BESIII collaboration also observed the cross section enhancement [2]}. The non-vanishing cross section near threshold as well as the wide-range plateau have led to various theoretical interpretations, including i) final-state interactions [3]}, ii) bound states or meson-like resonances [4]} and iii) an attractive Coulomb interaction [5]}. Recently, the BESIII collaboration has observed the non-zero cross section near threshold in the process \(e^{+}e^{-}\rightarrow \Lambda \bar{\Lambda }\)  [6]}. Naturally, it is also interesting to explore the production behavior of \(\Lambda _{c}^{+}\) , the lightest baryon containing the charm quark. Previously, the Belle collaboration measured the cross section of \(e^{+}e^{-}~\rightarrow ~\Lambda _{c}^{+} \bar{\Lambda }_{c}^{-}\)  using the initial-state radiation (ISR) technique [7]}, but the results suffer from significant uncertainties in CM energy and cross section. Therefore, near \(\Lambda _{c}^{+}\bar{\Lambda }_{c}^{-}\)  threshold, precise measurements of the production cross section and EMFF ratios are highly desirable.
